Production of light-conducting glass fibers by vapor partial pressureatmosphere

ABSTRACT

A GLASS FIBER CONTAINING GLASS-FORMING AND GLASS-MODIFYING OXIDES IS MAINTAINED AT A TEMPERATURE ABOVE ITS STRAIN POINT AND UNDER A VACUUM FOR A CERTAIN TIME THEREBY TO HAVE THE MODIFYING OXIDE VAPORIZE OFF THE FIBER WHEREBY THE FIBER HAS SUCH A REFRACTIVE INDEX DISTRIBUTION, IN A CROSS SECTION THEREOF TRANSVERSE TO THE DIRECTION OF LIGHT ADVANCE THERETHROUGH, THAT THE REFRACTIVE INDEX DECREASES CONTINUOUSLY FROM THE CENTER TOWARD THE OTHER PERIPHERY OF THE CROSS SECTION.

REFRQGTWE INDEX DISTRIEUTION DSTWEUTIOH apci, assigner to Nipuon Nippon Scioc application Continu: t o

. .critic-r2 May ili, 'iV/'2,

Sdllifi, Ser. No.

Ciairns prio.

ty, appli-:ration Japan, Get. 3, F568,

Ent, Cl, @63h 15/00; Fide N06 US. Cl. c45-37 6 Claims 0F THE DSCLGSURE GRSSE-REFERENCE TO RELATED APPLCATIONS This applicatie is a continuation-impart of my application Ser. No. 861,904, filed Sept. 29, i965), entitled Production ot Light Conducting Glass Fibers, and now abandoned.

BACKGRGUND OF THE INVENTXON This invention relates generally' to materials and structures through which light and images can be conducted and more particularly to light-couductin3` glass tibers or filaments. More specifically, the invention concerns a method of producing light-conducting glass fibers each exhibiting a refractive in ex distribution wherein the index decreases in a continuous manner outward from the center in cross sections o1? the ber perpendicular to the intended direction of advance of conducted light.

A light-conducting fiber known heretofore consists, essentially, of a core body for light conduction havingy a relatively high refractive index and a coverinrf layer having a relatively low refractive index and coveri 3 the core body. An interface is formed between the core structure and the covering layer. W en a light beam is introduced into one end of the core body at an angle grcaterthan the critical reflection angle of this interface, this light beam is repeatedly reflected from the interface and is thereby conducted through the liber core body.

However, such a clad-type, light-conducting liber Of known type wherein reliection is utilized to conduct the light has various drawbacks, the most serious oi which are as follows.

As an incident light beam introduced into the fiber advances by undergoing; repeated total reflection, diterenccs in the lengths of light paths between the il'nt rays of the beam develop, so that lags in phase velocities occur when the light beam leaves the fiber. When such lags in phase velocities are present. it becomes dillicult to transmit liebt signals varyinp at hiel# speed when the iight-conducting fiber is to be utilized for communication depending on light. l

Furthermore, as the light beam introduced 'nto the fiber advances as it is rcilectcd at the interface, the width thereof progressively s, and. at the same time, rc flecton loss urs at; the interface. Thi result also becomes a cri of impairment oi the elhcicncy of light cornninnication.

As means for conducting images or pictures, optical fiber plates and optical fiber bundles each consisting esse tially of a large number of clad-type optical fibers in he desired arrangement are being used. Each of these fract vc index and a cover layer of lower refractive index cove g the core body.

ln image-conducting means of this character, however, the individual optical 'libere merely conduct light as spots, and, accordiug'i thc resolution of the entire means is determined by the diameter of the optical ilbers. While the resolution can be increased to a certain degree by using fibers of small diameter, there is a lower limit to the liber diameter which can be obtained, it being extremely dii'i cult to produce optical iibers of diameters below 10 microns, whereby there is also a limit to the resolution which can be attained. Furthermore, the smaller the diameter of the Optical fibers is, the more complicated will the work of producing.v the image-conducting structure from these fibers be, whereby the eiiciency of this process will be low.

SUMMARY 0F THE INVENTION lt is an object of the present invention to provide a method of producing light-conducting glass fibers in which lag in phase velocities in a light beam at the exit end of the fibers and spreading of width and reflection loss of the light beam are prevented thereby to provide light-conducting tibcrs highly suitable for use in ultrahigh-specd, light-pulse communication and in ultra-high speed, las-cr pulse amplification.

Another object of the invention is to provide a method of producing light-conducting glass tlbers or filaments suitable for use in the abrication of image-conducting structures of simple construction, and a single ber of which is capable of conducting images.

According to the present invention, briefly summarized, there is provided a method of producing lightnconducting glass fibers in which a glass iiber containing at least: one glass-forming oxide and at least one glass-niodif5 i oxide is subjected to a temperature above the strain point of the fiber and an atmosphere having a vapor pressure which is lower than the saturated vapor pressure of said glass-modifying oxide at said temperature, both maiutained for a substantially longl period thereby to cause Athe iiber to have a refractive index distribution in a cross section thereof perpendicular to the direction of light advance therethrough wherein the refractive index decreases continuously from the center toward the periphery of the cross section.

The nature, principle, detailsand utility of the invention will be more clearly apparent from the following detailed description beginning with general considerations and concluding,7 with specific examples of practice constitutingY preferred embodiments of the invention, when read in conjunction with the accompanying drawing.

BRlEF DESCRIPTION OF THE DRAWING in the drawing:

FIG. l is a diagrammatic side view indicating the manner in which light is conducted through and by a light-conductingr liber of known clad type;

FiG. 2 is a similar view indicating the manner in which light is conducted tlirouf i and by a glass liber in accordance with the method of the invention',

NG. 3 is a dianramrnaulz: side view indicating the inanner in whia'n an nuage is conducted. through a glass liber produced according to the method of the invention;

FIG. 4 is a diagrammatic illustration ot' conccntration distribution of and T120 in l fibers consists of a lighhconducting core body of high re-A FIG. 5 is a diagrammatic 'illustration or the refractive index distribution in a cross-section of glass fiber groduccd according to the invention.

DETAILED DESCRHTIGN As mentioned brieiiy hereiubeforc and as indicated in FIG. l, a light-conducting ber of known type consists essentially of a core body l of a/relativcly high refractive index and a covering layer 2 of a relatively low retractive index covering the core body, an interface-'being formed therebetween. An incident light bcaln 3 introduced into the core body through one end thereof at an angle greater than the critical rellcction angle or this interface is conducted through and along the core structure l. as it is repeatedly reilected from the interface.

In contrast, when an incident light beam is introduced into one end of a light-conducting liber #i as shown in FIG. 2 and having a refractive index distribution wherein the index increases progressively inward from the outer surface of the liber, as in a glass tiber produced according to the invention, the incident light 5 advances through the iibcr i without being retlectcd at the outer surface of the fiber. Therefore., phasevelocity lag and width spreading of the light beam and light reflection loss are substantially reduced.

This highly desirable performance is due to a principle which is similar to that oi a so-called gas lens. A glass fiber in which the refractive index in a cross section thereof is radially symmetrical about the center ot the section and increases progressively inward from the outer surface (periphery of the cross section) is highly desirable since phase-velocity lag at the light exit and of the liber and width spreading of a light beam being conduc-ted, can be substantially reduced.

It is most desirable that the above mentioned refractive index distribution be representable by a quadratic curve of the form wh ere:

radial direction from the center of pressed in terms of mm. (millimeter).

(These symbols r, n, n,and a are used hereinafter in accordance with the above definitions.) When an incident light having a constant pulsewidth is introduced into a glass ber having the above defined refractive index distribution, the light is conducted through the fiber as it maintains the constant pulse width without phase-velocity lag and leaves the liber from thc exit end thereof.

When this light-conducting fiber is physically curved until it assumes a radius of curvature less than a certain limiting value, rays of an incident light beam entering the bcr at one end thereof are reflected by the outer surface thereof or escape out of the liber. This limitingy value of radius of curvature is determined by the refractive index distribution Within the liber. That is, this limiting radius or curvature ordinarily decreases with increase in the refractive index gradient.

The manner in which an optical fiber produced in accordance with the invention conducts an image is illustratcd infllG. 3, in which the optical liber c'. having in a cross section perpendicular to the intended direction Aof advance of incident' light a refractive index distribution fiber, and cach light ray at. 'ences with a sinusoidal 'ave equat ion from wherein the intrinsic or natural wavelength S is 21r/2\/2r1, 'whereby 'a real image is formed outside of the liber 6.

While the real image S is described above and indicated in FIG. 3 as being formed outside of the fiber 6, it is also possible to formA 'the image the planeA of the. light exit surface of the optical fiber 6 by suitably adjusting the length of the ber and the distance between. the object 7 and the optical ber t3. It is possible, furthermore, to adjust the magnification or reduction.

The refractive index of glass is dependent; principally On the composition of that glass. Accordingly, a glass structure in which the refractive index therewithin va progressively can be obtained by causing the glass to have a glass composition distribution wherein the composition differs progressively. Furthermore, a light-conducting glass liber in which the refractive index increases progressively inward from the outer surface can be obtained by causing a glass liber to have a glass composition distribution wherein the composition differs progressively from the outer surface toward the interior of. the liber. l-lowcver, glass structures, particularly glass Fibers, having glass composition. distributions wherein the relracn tive index varies progressively could not be easily produced heretofore.

In accordance with the present invention, there is provided a method of producing glass fibers each having a refractive index distribution in a cross section perpendicular to the direction of advance ot* light within the glass liber in which the relationship nzna (l-ar2) is substantially satislied, whereby the glass tibcrs are cap-able of accomplishing ultra-high-speed, light pulse communication, ultra-high-speed, laser pulse amplification, and image conduction.

This method of the invention can bc practiced, in eral, by forming a glass ber composed essentially of or more glass-forming oxides and one or more ;smodifying oxides and exposing the glass liber thus formed to an elevated temperature aud an atmosphere having a vapor pressure which is lower than the saturated vapor pressure of said glass-modifying oxide at said temperature such as a high degree of vacuum by maintaining the fiber for a long time in a furnace under a. high vacuum at an elevated temperature above the strain point and preterably below the softening point of the glass liber. The glassxnodifying oxides which is present ucar the outer surface of the fiber are thereby caused to vaporize, and a concentration `gradient thereof in directions within the fiber cross sections is produced. As a result, a glass liber having a refractive index distribution in cross sections perpendicular to the light advance direction which substatitially satisfies the equation 11:;10 (1-ar2) is produced.

In general, cations ot larger ratios of electronic pola ability to (ion radius)3 within a glass have a tendency to contribute more greatly to increase in refractive index. That is, this tendency in the case of monovalent cations is ot the sequence: Tl li l Na=Rbln the case of divalent cations, the relationship thcrco in the order of degree of contribution toward increase in the glass reractive index is: Pb Ba. Cd Sr Ca Zn Be Mg- Physical substances (solids and liquids) respectively have characteristics vapor pressures. In general, these pour pressures increase exponentially with risc in ternperature. Futherrnore, the rate. of Vaporization of a physical substance increases whcn :nat substance is surrounded by a vacuum 0r an atmosphere having a vapor bressure lower than the saturated vapor pressure at' "ven temperature of the substance, and this rate increases withA the degree or". vacuum.

When a substance composed of complicated constituents, such as anlass. is placed under conditions co to cvanoratioit, such as high temperature and hl n vacuum', the vaporlzation from this substance is auch that'. specitre constituents evaporate in particularly larry? n, n-

il il Nif? estaret '.5 titles since the vapor pressure of the various constituents of the substance differ greatly.

Oxide glasses contain glass-formi-g oxides and glassmodifyiue oxides in i form distributions, but glassoxidcs are in general, more vaporizablc than glasses after "-naorization of :ral has lower refractive in ling: oxides, and oxides will in n e 1 m the original t This phenomenon of invention, a feature of t.' containing glass-forming and glaswnodifying oxides undcr conditions of elevated temperature and high vacuum thereby to cause the `L to evaporate.

Glassrnodifying oxides have rn rates than glass-forming oxides. :or example, when e. glass comprising SiOZ which is a glass-form' oxide and PDO which is a g -modifying Oxide is heatcd at a tcmperature of approximately 700 C. under vacuum, the rate of vaporization out of the glass of Pb@ is a n 'llion tintes as large a perature, ,ibO '.y have saturated vapor pressure of approximately 4i X 10-3 mm, and SiO: may have saturated vapor presurc of approximately 3 x lG-9 mm. l-lg.

When a glass fiber which contains a glassfcrtning oxide s l:ss-rnodiff/ing` oxide 'in uniform concentrations within ti e glass and which has a uniform refractive index throuf'iout the fiber is pl and h h vacuum, the glass face of the fiber ywill vaporize off the fil; periphery surface thereof, since the satu ed vapor pressure of the glass-modif fing oxide is highcl than the pressure of the vacuum or gaseous atmosphe e surrounding the fiber, or, more precisely, than the partial pressure of the vapor of the gl modifying oxide in the vacuum or the nf. atnio lere which comprises the. vapor of the m difyirg om' e.

Once the concentration of the modifying oxide near the surf ce of the fiber is lowered by the vaporization, the modifying oxide remaining within the interior of the fiber will move by diffusion toward the surface so as to compensate for the difference in concentrations of: the modifying oxide at the sur e and in the interior of the fiber. When the fiber is placed under such conditions for certain duration of time, the concentration of the modifying oxide nearer surface is decreased more intensely than that in the interior or the glass, and the concentration of a forming oxide nearer the surface of the fiber is on the contrary increased more intensely correuonding to the decrease in concentration of modifying, ox at that place. Thus, the refractive index of glass nearer the surface of the fiber is much lower than the original one. ln a crossscction of the fiber perpendicular' to the central axis thereof, concentrations of the modifying oxide and the forming oxide continuously decreases and ir respectively, from the central axis toward the peripl i of the fiber, and, since a glass part containing a modifying; oxide in a lower concentration and a forming oxide in a higher concentration has a lower refractive index than the original glass, the refractive index continuously decreases from the central axis towardthe surface of the fiber.

In the case where the duration of time of such heat treatment under vacuum is relatively short, the concentration gradient of modifying and forniA .c oxides an thus the refractive index gradient will be produced only at the sur face of the fiber, and the concentrations of modifying and formingr oxides and refractive index will remain substantially unfit' ted in a deeper part of the glass fiber. In

` ere the duration of time is re ivelv long, con

modifyi' sarl forming c re z. 't cd from the original ones even at the cent al ai s, resneetivcly, and refractive index at the center axis andan ld at an elevated temperature -modifying oxide near the surthrough the inodifyinT oxide within the fiber will .'acoric olf the liber, and the c that of SiO2 or even larger. At this terrtf forming oxides within the glass fiber are not produced amply enough to establish a required refractive index gradient.

Thus, when the duration of time is so selected as to produce within the glass liber such concentration of modifying oxide that it is substantially the same as the original one r the center axis and is slightly lowered at a place slightly distant from the axis or that it is lowered at the center axis, the concentration of modifying oxide will clecrcase continuously from the central axis toward the outer surface of the fiber in proportion to the square of the radial distance from the central axis of the fiber and the concentration of forming oxide will thus increase continuously from the center toward the outer surface of the ber in proportion to the square of the radial distance frorn the een er axis of the fiber. Since refractive index. of a glass a preferable. Vrefractive index gradient, the concentration of modify/liar oxide at the outer surface can be substan- 1 zero if desired.

While the glass-modifying oxides have much higher vaporiziation rates than the `r.'lass-forrning oxides, there are not little differences in the vaporization rates even among, the glass-modifying oxides. In the selection of the glasstnodifying oxides, features thereof such as vaporizatiou rates, degree of contribution to the refractive index, and suitability of the diffusion within the glass must be considered, l have found that T120 and Css@ among nionovalent. glass-modif g oxides and PbO and CdG among divalcnt glass-modifying oxides are particularly convenient because of their great contribution to the glass refractive index and their high vaporization rates.

The process temperature. must be sufficiently high to cause vaporization of the glass-modifying oxides and yet must be sufficiently low to preserve the original shape of the fiber. Therefore, it is necessary that this temperature be above the strain point and preferably below the softening point of the glass tibet'..The degree of vacuum used in the process should be made as high as possible that is` for example, a pressure lower than 10-2 rnm. Hg, since the evaporation is increasingly porinoted by increasing the degree of vacuum.

When a glass fiber containing a glass-modifying oxide which is capable of contributing greatly to the refractive index and, moreover, has a high vaporization rate, is maintained for a suflicient time in a high vacuum at a temperature above the strain point and preferably below the softening point, in accordance with the invention, the evaporation of the glass-modifying oxide which is present. near the outer surface gives rise to a difference in concentrations of this oxide between the interior and outer sur .face of the glass fiber, and diffusion of this oxide occurs within the glass fiber from the interior toward the outer surface thereof.

r,The distribution of concentration of the glass-modifying oxide in a cross section of the glass fiber perpendicular to the light advance direction substantially confort s to a diffusion equation with the result that a glass fiber in which the aforementioned refractive index distribtuion in a transverse section substantially satisfies the equation 11:11 (1-ar-).

For the light-conducting7 glass liber produced by the rr-ethod of the invention, silicate classes, berate glasses, phosphate glasses, and other o' c glasses can be used.

itt/'hen :zu incident light beam is introduced into t cud of a tht-f.' n :tim:y glass fiber produced accord to the invenilon, the without the within the in the light ad.

That is, the vincide-nt licht adva dire non as it curves tov-.fard thc sido sensei il?! of higher refractive index. Accordingly, by using the lightcoudncting hner of the invention, it possible to curve the light advance direction.

Furthermore, a light-conducting glass i'ihcr having a refractive index distribution in a cross section perpendicular to the light-conducting direction which is radially symmetrical about th: liber center line or central airis and is such that the refractive index decreases with di ance away from the center line can be caused to function as a Convex less such as that for focusing light beams.

Since an incident light benin advunces throne' the glass liber of tl Y there is no phase velocity lug; in the light beam exi. from the liber, and, moreover, sprca g of the light m width is prevented. Accordingly, it is possible to utilize conducting glass fiber of the invention in light continui tion to tran. tit eiliciently licht signals varying at high speed. By pro rg a. light-c. nductinp glass fiber of the invention in one part of a light-conducting; p light-communication systern and utilizing the tibility possessed by the ber, the position aud direction of light leaving the exit surface of the liber can he adju d at will.

In contrast. to light-conducting glass fibers of known clad type, cach of which always required a glass covering layer for reilection, the light-conducting; glass of the invention does not always require a covering layer or reflection. Accordingly, a feature of the fiber oi the invention is that the etlective arca for light conduction is large, and, moreover, the production thereof is facilitated.

The light-conducting glass liber ot the invention can also be coated over its outer surface, in accordance with necessity, '\vith a substance of lower reti-active index, a lightabsorbent substance, or a light-tellective substance. Furthern'tore, it is also possible to assemble a plurality of thee fibers into a fiber bundle or a fiber plate. The fibers or" this invention can be practically applied to a wide variety of light-conducting devices and apparatuses including those for communication by laser and other `kinds o light and those for various modes of image conduction.

The terra fiber or lainent as herein used should be interpreted as meaning any physical structure having a cross section which is relatively small in relation. to the ength thereof irrespective o the shape of the cross section.

ln order to indicate still more clon ly the nature and utility of thc present invention, the following examples of practice constituting preferred embodiments thereof and results are set forth, it being understood that these eX- amples are presented as illustrative only and that they are not intended to iirnit the scope ot the invention. Throughout these examples, all percentages are by weight.

EXAM PLE 1 A glass liber of 0.1 rnrn. diameter and a composition essentially of 50 percent of T12() and 50 percent of SiOg was prepared. The `glass fiber had a refractive index of 1.58, r1. strain point (the temperature at `which the glass viscosity is 10H5 poiscs) of 430 C., and a softening point (the temperature at which the glass viscosity is 10V-5 `poises) of 630 C.

This cms, liber was suspended within an electric furnace which could hc hermetically scaled, und the furnace tcmperature was maintained at approximately 470 C. The internal pressure of the furnace was reduced to approxh mately 104 mm. Hg by means ot' a vacuum pump conneet-ed to the furnace. At these values of temperature and pressure the ass fiber is thus maintained at n temperature above the s in point and in an :timos here wherein the partial pi :1re of the 'llgG component below the saiurutcd vapor pressure of the T120 cornpount, so that vonorization of the 'llg'j component occurs. vaporization t the rcsultaot entr-rrd dill'usiou of the llzO produces a concentration di r-ution of the components as iilustrzitcrl in FG. Il. The glass fiber was continuously subjected to these conditions of temperature and pressure for 16 hours.

The glass liber thus processed had a. refractive iurisY ol' 1.58 at its center line part and a refractive index o 1.51 at the outer surface. The glass composition at the center of the liber was substantially the same es the original one, and the glass composition at the surface of the such that concentration of .fl-O was approximately 0% and of SiOg was approximately 100% and that concentration of T120 and SiOz decreased and increased, respectively, from the center toward the surface of the fiber substantially parabolically. lt was found also that the rc- Jfructive inde-x distribution over e cross section perpendicular to the liebt advance direction was such that the refractive index decreased substantially parabolically from the center toward the outer surface of the ber as shown tli'lcrarrlrnatically in FlG. 5, and the refractive index gra t was expressed by the aforementioned equation in which the constant rz was 17.7 mnt-2.

A part of a piece of this glass fiber of a length of approximately 10 crn. was deflected into curved shape of a radius of curvature ot 1 cm., and incident l'cht beam of width of approv 'nately 0.01 mm. was projected into the central part of one end surface of this glass liber, whereupon the light beam advanced through and along the glass liber interior along an undulating path and, more-- over, Without being rellected by the fiber outer surface 'until the light bcum reached the other end ot, the ber.

lt vas found that the width of the light bcani thus reaching this other end of the ber was substantially equal to the width of the light beam at the time ot' its incidence.

*XAMPLE 2 A glass liber of 0.1 mm. diameter and a composition of 55 percent of PbO and 45 percent of SiOz and having a refractive index of 1.63, a strain point of 580 C., and a softening point of 760 C. was prepared. rlisis glass fiber was suspended within an electric furnace which could he hcrnctically sealed, and the 'furnace temperature was maintained at approximately 700 C. vJith the fiber in this state, the furnace internal pressure was reduced to approximately 10@ mm. wh' is lower than the saturated vapor pressure of Pb@ `vithin the glass at the furnace temperature, namely 4 10'3 rnin. Hg, by rneans of vacuum pump connected to the furnace, and the glass 'oer was maintained for 24 hours under these conditions of temperature and pressure, during which the Pb() component vaporized off the liber through the outer surface thereof,

AAs a result of this process, the glass fiber was found to have a refractive index ot 1.63 at its center line part and of 1.53 at the outer surface. The glass composition at the center' line part was substantially the same as the original one, and the glass composition at the outer surface was substantially Zero percent of PbO and substantially 100% of SiO2, the concentration of PbO and of SiOg decreasing and increasing, respectively, from the center line toward the outer surface substantially parabolicnlly. It was found additionally that the refractive index distribution over a cross section perpendicular to the light; advance direction was such that the refractive index de creased substantially parabolically from the center toward the outer surface o the liber whereby the constant a of the equation was 24.5 mur-'2.

A part ol: a piece of this -class fiber of a length ot approximately 10 cm. was dellectcrl into a curved shape o a radius of curvature of l cm., and an incident light boum of :t width of approximately 0.01 .ru-fri. was projcc ed into the central `art ot one end surface ol this glass liber, whereupon the light beam advance; through and al the liber interior along :tn undulating path end, tu' without bcingellcetetl by the liber outer sui-fac.. light beam reached the other end otf the liber.

lt. was found that the width ol? the l t equal to the width of tne light beam at the time of its incidence.

EXAMPLE 3 A glass fiber of 0.1 mm. diameter and a composition of 16 percent of TIQO, 48% of SiOz. 24% of PbO, and 12% of NagO, and having a refractive index of 1.60, a. strain point of 360'J C., and a softening point of 540 C. was prepared.

This glass ber was suspended within an electric furnace which could be herinctically sealed, and the furnace tenipcrature was maintained at approximately 430 C. rthe internal pressure of the furnace was reduced to approximately l()H4 rnm. Iig by nit-.ans of a vacuum pump con nected to the furnace. The glass fiber was continuously subjected to these conditions of temperature and pressure for 4() hours. he pressure, 1t)Ax inni. Hg, is lower than thc saturated vapor pressure of T120 within the glass at the furnace temperature, approximately l-2 mm. Hg, and thus vaporization of 'i120 component principally occurred.

The glass fiber thus processed had a refractive index of 1.59 at its center line-part and a refractive index of 1.56 at the outer surface.

The glass composition at the center of the fiber was 13.0% of T120, 49.5% ot SiOg, 25.0% of PbO. and 12.5% of NaZG, and the glass composition at the surface ot the tiber was 3.0% of T120, 55.5% o SiO2, 27.7% of PbO, and 13.8% of Na2O, whereby the concentration ot T120 decreased from the center toward the surface substan tially parabolically and the concentrations of SiOg, PbO and Naz() increased from the center toward the surface substantially parabolically.

It was also found that. the refractive index distribution over a cross section perpendicular to the light advance direction was such that the refractive index decreased substantially paraboiically from the center toward the outer surface of the fiber, whereby the constant a of the equation was 7.5 min-T'.

A part of a piece of this glass liber of a length of approximately cru. was deected into a curved shape of a radius of curvature ot 1 ern., and an incident light beam of a width of approximately 0.01 mm. was projected into the central part of one end surface of this glass ber, whereupon the light beam advanced through and along thc glass iibcr interior along an undulating path and, moreover, without beinn retlected by the liber outer surface until the light beam reached the other end of the fiber.

1t was found that the width of the light beam thus reaching this other end of the fiber was substantially equal to the width of the light beam at the time of its incidence.

What is claimed is:

1. A method of producing a. light-conducting glass liber having a principal light-conducting center' axis and having a distribution of refractive index wherein said index decreases continuously from the center axis toward the outer surface of the liber in any cross section thereof perpendicular to the axis, which comprises: providing a glass liber having a uniform refractive index tlierewitliin and comprising at least one tirst oxide and at least one second oxide, each of said tirst and second oxides being initialiy distributed within the glass liber with uniform concentrations, said second oxide being sucll that it is more vaporiL/ ablc oft the glass than said first oxide and that it is conducive to lowering the refractive index of the glass when it has vaporized oit the glass; and maintaining, said glass iibcr at a temperature above the strain point centration distribution of said first and second oxides within thc glass fiber such that in any cross-section perpendicular to the center axis of the fiber said concentration ot said first and second oxides respectively increases and. decreases continuously from the center axis toward the surface of the fiber and that said concentration distribution produces a corresponding refractive index distribution, whereby said refractive index decreases continuously from the center axis toward the surface of the fiber.

2. A method of producing a light-conducting glass fiber as set forth in claim '.i, in which said temperature is below the softening temperature of the glass fiber.

3. A. method of producing .light-conducting glass bers as set forth in claim in which said second oxide is at least one oxide selected from the group consisting oi TlgO, CszO, PbO, and CdO, and said first oxide is Si02.

it. A method of producing light-conducting glass fibers as set forth in claim 1, in which said gaseous atmosphere has a pressure lower than l0*2 znrn. Hg.

5. A method of producing light-conducting glass fiber as set forth in claim 1, in which said time is so selected as to produce in a cross-section of the fiber perpendicular to the center axis of the iiber such concentration of said second oxide that it is substantially the saine as the original one at the center and is slightly lower than the orif'inal one at a place slightly distant from the center, whereby said refractive index distribution substantially satisfies the equation: iz=no (l-ar2), wherein r is the radial distance from said axis of the bcr, no is the rcfractive index of the glass ber at said axis, lz is the refractive index oi the glass liber at the distance r, and c is a positive constant,

6. A method of producing light-conducting glass fiber as set forth in claim l, in which said tinte is so selected as to produce in a cross-section of the fiber perpendicular to the center axis of the fiber such concentration of said second oxide that it is lowered at the center, whereby said refractive index distribution substantially satisfies the equation: 11:11 (1-ar2, wherein ris the radial distance from said axis of the fiber, no is the refractive index of the glass liber at said axis, n is the refractive index of the glass fiber at the distance r, and a is a positive constant.

Reterences Cited UNITED STATES PATENTS FRANK W. MIGA, Primary Examiner U.S. Cl. XR.

--3, 4, 30, Dig. 7; 106--50 

